ASTM E2235-03
(Test Method)Standard Test Method for Determination of Decay Rates for Use in Sound Insulation Test Methods
Standard Test Method for Determination of Decay Rates for Use in Sound Insulation Test Methods
SCOPE
1.1 This test method covers the measurement of sound decay rate in rooms and the calculation of the sound absorption of the room and its contents. The sound absorption so calculated may be used in calculations in sound insulation test methods.
1.2 The method shall be used only in conjunction with other test methods where the logarithm of the sound absorption is used in formulas. It is not sufficiently precise for use in situations where room sound absorption is to be used without taking logarithms.
1.3 For laboratory measurements of the sound absorption of materials and objects, Test Method C 423 should be used.
1.4 This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.
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NOTICE: This standard has either been superseded and replaced by a new version or withdrawn.
Please contact ASTM International (www.astm.org) for the latest information.
Designation:E2235–03
Standard Test Method for
Determination of Decay Rates for Use in Sound Insulation
Test Methods
This standard is issued under the fixed designation E 2235; the number immediately following the designation indicates the year of
original adoption or, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. A
superscript epsilon (´) indicates an editorial change since the last revision or reapproval.
INTRODUCTION
This test method is part of a set of methods used to evaluate the sound-insulating properties of
building elements. It is intended for use in conjunction with methods for measuring the transmission
of sound through a partition or partition element in a laboratory or in a building. These methods
include the laboratory measurement of airborne sound transmission loss of building partitions and
elements (Test Method E 90E90), the measurement of sound isolation in buildings (Test Method
E 336E 336), the laboratory measurement of impact sound transmission through floors (Test Method
E 492E 492), the measurement of impact sound transmission in buildings (Test Method
E 1007E 1007), the measurement of sound transmission through building facades and facade elements
(Guide E 966E 966), and the measurement of sound transmission through a common plenum between
two rooms (Test Method E 1414E 1414).
1. Scope C 634 Terminology Relating to Environmental Acoustics
E90 Test Method for Laboratory Measurement of
1.1 This test method covers the measurement of sound
Airborne-Sound Transmission Loss of Building Partitions
decay rate in rooms and the calculation of the sound absorption
and Elements
of the room and its contents. The sound absorption so calcu-
E 336 Test Method for Measurement of Airborne Sound
lated may be used in calculations in sound insulation test
Insulation in Buildings
methods.
E 492 Test Method of Laboratory Measurement of Impact
1.2 The method shall be used only in conjunction with other
Sound Transmission through Floor-Ceiling Assemblies
test methods where the logarithm of the sound absorption is
Using the Tapping Machine
used in formulas. It is not sufficiently precise for use in
E 966 Guide for Field Measurement of Airborne Sound
situations where room sound absorption is to be used without
Insulation of Building Facades and Facade Elements
taking logarithms.
E 1007 Test Method for Field Measurement of Tapping
1.3 For laboratory measurements of the sound absorption of
MachineImpactSoundTransmissionthroughFloor-ceiling
materials and objects, Test Method C 423C 423 should be
Assemblies and Associated Support Structures
used.
E 1414 Test Method for Airborne Sound Attenuation be-
1.4 This standard does not purport to address all of the
tween Rooms Sharing a Common Ceiling Plenum
safety concerns, if any, associated with its use. It is the
2.2 ANSI Standards:
responsibility of the user of this standard to establish appro-
S1.4 Specification for Sound-Level Meters
priate safety and health practices and determine the applica-
S1.6 Standard Preferred Frequencies, Frequency Levels,
bility of regulatory limitations prior to use.
and Band Numbers for Acoustical Measurements
2. Referenced Documents
S1.11 Specification for Octave-band and Fractional-Octave-
Band Analog and Digital Filters
2.1 ASTM Standards:
C 423 Test Method for Sound Absorption and Sound Ab-
3. Terminology
sorption Coefficients by the Reverberation Room Method
3.1 Definitions of the acoustical terms used in this test
method are given in Terminology C 634C 634.
3.2 Definitions of Terms Specific to This Standard:
This test method is under the jurisdiction of ASTM Committee E33 on
EnvironmentalAcousticsandisthedirectresponsibilityofSubcommitteeE33.01on
Sound Absorption.
Current edition approved April 10, 2003. Published June 2003. Available from American National Standards Institute (ANSI), 25 W. 43rd St.,
Annual Book of ASTM Standards, Vol 04.06. 4th Floor, New York, NY 10036.
Copyright © ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.
NOTICE: This standard has either been superseded and replaced by a new version or withdrawn.
Please contact ASTM International (www.astm.org) for the latest information.
E2235–03
placing sources in trihedral corners of the room will be adequate.
3.2.1 output interval, Dt;[T];s—of a real-time analyzer,the
time between successive outputs of sound pressure levels
7. Sound Source Positions
during a single decay measurement.
7.1 At least one source position shall be used in the room.
4. Summary of Test Method
NOTE 3—Where more than one source position is used, decay rate data
4.1 Sound decay rate in rooms is a function of frequency so
may be collected for each source position in sequence and then the decay
measurements are made in a series of frequency bands. Bands
rates averaged. Alternatively, multiple loudspeakers may be activated
of random electrical noise are used as signals to drive loud-
simultaneously. If this is done, the sound power emitted by the loud-
speakers in the room until the sound pressure level reaches a speaker sources should be approximately equal. Separate electronic noise
generators and amplifiers for each system are not necessary.
steady state. When the sound is then turned off, the sound
pressure level decays at a rate determined by the sound
8. Electrical Signal
absorption in the room. The decay rate is measured in each
frequency band by measuring the slope of a straight line fitted 8.1 Theelectricalsignalfedtoeachpoweramplifiershallbe
to the average decay curve. The absorption of the room and its a band of random noise with a continuous spectrum covering
contents is calculated from the Sabine formula: the frequency range over which measurements are made.
Vd
A 5 0.921 (1)
9. Frequency Range
c
9.1 The frequency range of the measurements shall be that
where:
2 specified in the companion standard for which the measure-
A = sound absorption, m ,
3 ments are being made.
V = volume of reverberation room, m ,
9.2 Bandwidth—For each test band, the overall frequency
c = speed of sound, m/s, and
response of the electrical system, including the filter or filters
d = decay rate, dB/s.
in the source or microphone systems, shall satisfy the specifi-
5. Significance and Use cations given in ANSI Specification S1.11 for a one-third
octave band filter set, Order 3 or higher, Type 1.
5.1 Several ASTM test methods to evaluate the sound-
insulating properties of building elements require the measure-
NOTE 4—The shape of the filter response curve can influence the
ment of room sound absorption as part of the procedure. The
minimum decay rate that can be measured. This problem is dealt with by
room sound absorption in these standards appears in an the requirement in 13.5.
equationintheform10log(x/A),where xisaquantitywiththe
10. Microphone Requirements
same units as A,m . Room sound absorption is calculated from
the decay rate using Eq 1.
10.1 A microphone used to measure decay rate shall be
5.2 The requirements of this standard have been chosen so
omnidirectional with a 6 1 dB random-incidence amplitude
the uncertainty associated with the measurement of room
response within any one-third octave band for all frequencies
sound absorption will be acceptably small so long as the
and sound pressure levels used for decay rate measurements.
logarithm of the absorption is being used in calculations.
5.3 Other test methods should specify explicitly that they
11. Microphone Positions
make use of this test method.
11.1 Stationary Microphones:
5.4 Where measurement requirements in the parent standard
11.1.1 In the absence of an over-riding requirement in the
differ from those given here, the requirements in the parent
companion standard, the number of stationary microphone
standard shall be satisfied.
positions shall be at least three.
5.5 This method shall not be used when room sound
11.1.2 In the absence of an over-riding requirement in the
absorption or decay rate is to be used directly to satisfy some
companion standard, stationary microphone positions shall be
criterion, for example in a room that must not be overly
at least 1.5 m apart, and at least 0.75 m from any surface of the
reverberant so speech will be intelligible.
room.
NOTE 1—The uncertainty of the room sound absorption obtained will
11.2 Moving Microphones:
usually be too high and additional measurements are necessary.
11.2.1 Only one location of a moving microphone assembly
5.6 Any companion standard may specify the use of the
is required in the room.
procedures in this method for determining whether the decay
11.2.2 The length of the path for a moving microphone shall
rates in a room are slow enough to satisfy the requirements of
be that specified in the companion standard for which mea-
the companion standard. The measured decay rates s
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